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research article

A hybrid collocation-perturbation approach for PDEs with random domains

Castrillon-Candas, Julio E.
•
Nobile, Fabio  
•
Tempone, Raul F.
June 1, 2021
Advances In Computational Mathematics

Consider a linear elliptic PDE defined over a stochastic stochastic geometry a function of N random variables. In many application, quantify the uncertainty propagated to a quantity of interest (QoI) is an important problem. The random domain is split into large and small variations contributions. The large variations are approximated by applying a sparse grid stochastic collocation method. The small variations are approximated with a stochastic collocation-perturbation method and added as a correction term to the large variation sparse grid component. Convergence rates for the variance of the QoI are derived and compared to those obtained in numerical experiments. Our approach significantly reduces the dimensionality of the stochastic problem making it suitable for large dimensional problems. The computational cost of the correction term increases at most quadratically with respect to the number of dimensions of the small variations. Moreover, for the case that the small and large variations are independent the cost increases linearly.

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Type
research article
DOI
10.1007/s10444-021-09859-6
Web of Science ID

WOS:000646214100002

Author(s)
Castrillon-Candas, Julio E.
Nobile, Fabio  
Tempone, Raul F.
Date Issued

2021-06-01

Published in
Advances In Computational Mathematics
Volume

47

Issue

3

Start page

40

Subjects

Mathematics, Applied

•

Mathematics

•

uncertainty quantification

•

stochastic collocation

•

perturbation

•

stochastic pdes

•

finite elements

•

complex analysis

•

smolyak sparse grids

•

partial-differential-equations

•

polynomial interpolation

•

numerical-solution

•

thin-layer

Editorial or Peer reviewed

REVIEWED

Written at

EPFL

EPFL units
CSQI  
Available on Infoscience
June 5, 2021
Use this identifier to reference this record
https://infoscience.epfl.ch/handle/20.500.14299/178570
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